54 research outputs found

    Double-Spin Asymmetry in the Cross Section for Exclusive rho^0 Production in Lepton-Proton Scattering

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    Evidence for a positive longitudinal double-spin asymmetry = 0.24 +-0.11 (stat) +-0.02 (syst) in the cross section for exclusive diffractive rho^0(770) vector meson production in polarised lepton-proton scattering was observed by the HERMES experiment. The longitudinally polarised 27.56 GeV HERA positron beam was scattered off a longitudinally polarised pure hydrogen gas target. The average invariant mass of the photon-proton system has a value of = 4.9 GeV, while the average negative squared four-momentum of the virtual photon is = 1.7 GeV^2. The ratio of the present result to the corresponding spin asymmetry in inclusive deep-inelastic scattering is in agreement with an early theoretical prediction based on the generalised vector meson dominance model.Comment: 10 pages, 4 embedded figures, LaTe

    Measurement of the Proton Spin Structure Function g1p with a Pure Hydrogen Target

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    A measurement of the proton spin structure function g1p(x,Q^2) in deep-inelastic scattering is presented. The data were taken with the 27.6 GeV longitudinally polarised positron beam at HERA incident on a longitudinally polarised pure hydrogen gas target internal to the storage ring. The kinematic range is 0.021<x<0.85 and 0.8 GeV^2<Q^2<20 GeV^2. The integral Int_{0.021}^{0.85} g1p(x)dx evaluated at Q0^2 of 2.5 GeV^2 is 0.122+/-0.003(stat.)+/-0.010(syst.).Comment: 7 pages, 3 figures, 1 table, RevTeX late

    Measurement of the Neutron Spin Structure Function g1ng_1^n with a Polarized ^3He Target

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    Results are reported from the HERMES experiment at HERA on a measurement of the neutron spin structure function g1n(x,Q2)g_1^n(x,Q^2) in deep inelastic scattering using 27.5 GeV longitudinally polarized positrons incident on a polarized 3^3He internal gas target. The data cover the kinematic range 0.023<x<0.60.023<x<0.6 and 1(GeV/c)2<Q2<15(GeV/c)21 (GeV/c)^2 < Q^2 <15 (GeV/c)^2. The integral 0.0230.6g1n(x)dx\int_{0.023}^{0.6} g_1^n(x) dx evaluated at a fixed Q2Q^2 of 2.5(GeV/c)22.5 (GeV/c)^2 is 0.034±0.013(stat.)±0.005(syst.)-0.034\pm 0.013(stat.)\pm 0.005(syst.). Assuming Regge behavior at low xx, the first moment Γ1n=01g1n(x)dx\Gamma_1^n=\int_0^1 g_1^n(x) dx is 0.037±0.013(stat.)±0.005(syst.)±0.006(extrapol.)-0.037\pm 0.013(stat.)\pm 0.005(syst.)\pm 0.006(extrapol.).Comment: 4 pages TEX, text available at http://www.krl.caltech.edu/preprints/OAP.htm

    Flavor Decomposition of the Polarized Quark Distributions in the Nucleon from Inclusive and Semi-inclusive Deep-inelastic Scattering

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    Spin asymmetries of semi-inclusive cross sections for the production of positively and negatively charged hadrons have been measured in deep-inelastic scattering of polarized positrons on polarized hydrogen and 3He targets, in the kinematic range 0.023<x<0.6 and 1 GeV^2<Q^2<10 GeV^2. Polarized quark distributions are extracted as a function of x for up $(u+u_bar) and down (d+d_bar) flavors. The up quark polarization is positive and the down quark polarization is negative in the measured range. The polarization of the sea is compatible with zero. The first moments of the polarized quark distributions are presented. The isospin non-singlet combination Delta_q_3 is consistent with the prediction based on the Bjorken sum rule. The moments of the polarized quark distributions are compared to predictions based on SU(3)_f flavor symmetry and to a prediction from lattice QCD.Comment: 14 pages, 6 figures (eps format), 10 tables in Latex New version contains tables of asymmetries and correlation matri

    Erratum to: "Nuclear Effects on R=\sigma_L/\sigma_T in Deep-Inelastic Scattering" Phys.Lett. B475(2000)386

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    This erratum revokes the main conclusion of a Letter that reported measurements of cross sections for deep-inelastic scattering (DIS) of leptons on 3^3He and 14^{14}N targets, expressed as ratios of σA/σD\sigma_A / \sigma_D to the cross section on the deuterium target.Comment: 3 pages, 1 figur

    Padronização de técnica manual para obtenção de plasma rico em plaquetas de bovino

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    Resumo: Para padronização de uma técnica manual para a obtenção de plasma rico em plaquetas (PRP) autólogo em bovinos com custo reduzido (método manual) e de boa qualidade (capacidade de concentrar plaquetas, alta concentração de fatores de crescimento e contaminação reduzida com leucócitos e eritrócitos), que poderá ser utilizado como um agente modulador da resposta imune de vacas com diferentes enfermidades, 450 ml de sangue total de nove vacas clinicamente saudáveis e com perfil hematológico normal foi coletado em bolsas de sangue CPDA-1 e processado dentro de quatro horas após a coleta. O sangue foi separado em alíquotas para avaliar 8 protocolos (P) de centrifugação dupla que variaram quanto a velocidade e o tempo de centrifugação. A contagem de plaquetas, eritrócitos e leucócitos na suspensão obtida (PRP) foi realizada pelo método manual em câmara de Neubauer: P5 (400g e 800g ambos durante 10 min) foi o protocolo com maior número de plaquetas, seguido por P3 (120g e 473g ambos durante 10 min), P4 (300g e 640g durante 10 min cada), P6 (640g durante 10 min e 640g durante 5 min), P8 (640g durante 5 min e 120g durante 10 min) e P7 (720g e 720g durante 5 min) e diferentes (p<0,05) dos menores valores encontrados em P1 (120g e 240g, ambos por 5 minutos) e P2 (120g e 473g ambos por 5 min). Em relação aos eritrócitos, P8, P7, P6, P5 e P4 apresentaram menores concentrações e maiores valores (p<0,05) foram observados em P3 e P2. Menores quantidades de leucócitos foram observadas em P5, P6, P8 e P7 com o maior valor obtido em P2 (p<0,05). Todos os protocolos (P1 a P8) foram eficientes em concentrar plaquetas sendo o valor mais baixo (3,65±0,79) observado em P1. Em relação aos fatores de crescimento ao se mensurar TGF- 1, os protocolos P1 e P8 evidenciaram valores mais elevados. De acordo com os resultados obtidos os protocolos P5 e P8 apresentaram os melhores resultados para confecção de PRP bovino

    Techniques for the characterization of sub-10-fs optical pulses: a comparison

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